integration_da_add_material.info

ensemble
{
  ensemble_simulation true
  ensemble_size 3
  initial_temperature_stddev 5.0
  beam_0_absorption_stddev 0.05
}
experiment
{
  read_in_experimental_data true
  log_filename integration_da_add_material_expt_log.txt
  file integration_da_add_material_expt_pc_#camera_#frame.csv
  format point_cloud
  first_frame 0
  last_frame 0
  first_camera_id 0
  last_camera_id 0
  first_frame_temporal_offset 0.06
  estimated_uncertainty 1.0
}
data_assimilation
{
  assimilate_data true
  localization_cutoff_function gaspari_cohn
  localization_cutoff_distance 5.0e-1
  solver
  {
    max_number_of_temp_vectors 10
    convergence_tolerance 1.0e-8
  }
}

geometry
{
  import_mesh false ; Use built-in mesh generator
  dim 3 ; dimension of the domain
  length 100.0e-3 ; [m]
  height 20.0e-3 ; [m] In 3D, the third parameters is width
  width  100.0e-3
  length_divisions 3 ; Number of cell layers in the length direction
  height_divisions 3 ; Number of cell layers in the height direction
  width_divisions  3
  material_deposition true
  material_deposition_method scan_paths
  deposition_length 2.0e-3
  deposition_height 2.0e-3
  deposition_width 2.0e-3
  deposition_lead_time 1.0e0
  material_height 14.0e-3
}

physics
{
  thermal true
  mechanical false
}

boundary
{
  type adiabatic ; convective,radiative
}

refinement
{
  n_refinements 0 ; Number of time the cells on the paths of the beams are
                  ; refined
  time_steps_between_refinement 200000 ; number of time steps after which
                                       ; the refinement process is performed
}

materials
{
  n_materials 1

  property_format polynomial
  material_0
  {
    initial_temperature 285
    solid
    {
      density 7904; [kg/m^3] For now all the states needs to have the same
                    ; density.
      specific_heat 714; [J/kg K]
      thermal_conductivity_x 31.4 ; [W/m K]
      thermal_conductivity_y 31.4 ; [W/m K]
      thermal_conductivity_z 31.4 ; [W/m K]
    }

    powder
    {
      specific_heat 714; [J/kg K]
      density 7904; [kg/m^3]
      thermal_conductivity_x 0.314 ; [W/m K]
      thermal_conductivity_y 0.314 ; [W/m K]
      thermal_conductivity_z 0.314 ; [W/m K]
    }

    liquid
    {
      specific_heat 847; [J/kg K]
      density 7904; [kg/m^3]
      thermal_conductivity_x 37.3 ; [W/m k]
      thermal_conductivity_y 37.3 ; [W/m k]
      thermal_conductivity_z 37.3 ; [W/m k]
      ; Not all three states need to define the same properties or to exist
    }

    solidus 1675; [K]
    liquidus 1708; [K]
    latent_heat 290000 ; [J/kg]
  }
}

sources
{
  n_beams 1

  beam_0
  {
    type goldak ; goldak (laser) or electron_beam
    depth 3.0e-3 ; [m] maximum depth reached by the laser
    diameter 3.0e-3 ; [m]
    scan_path_file integration_da_add_material_sp.txt
    scan_path_file_format segment
    absorption_efficiency 0.6 ; number between 0 and 1 equivalent to
                              ; energy_conversion_efficiency * control_efficiency
                              ; for an electron beam
    max_power 900.0 ; [W], current * voltage for an electron beam
  }
}

time_stepping
{
  method forward_euler ; Possibilities: backward_euler, implicit_midpoint,
                        ; crank_nicolson, sdirk2, forward_euler, rk_third_order,
                        ; rk_fourth_order
  duration 2.0e-1 ; [s]
  time_step 2.0e-2 ; [s]
}

post_processor
{
  filename_prefix output
  time_steps_between_output 1
}

discretization
{
  thermal 
  {
    fe_degree 2
    quadrature gauss ; Optional parameter. Possibilities: gauss or lobatto
  }
  mechanical 
  {
    fe_degree 1
    quadrature gauss ; Optional parameter. Possibilities: gauss or lobatto
  }
}

profiling
{
  timer true
  caliper "spot(profile.mpi),loop-report,runtime-report"
}

memory_space host ; Always run on the host